Atjaunināt sīkdatņu piekrišanu

Modern Theory of Thermoelectricity [Hardback]

(Retired, Institute of Physics, Zagreb), (Adjunct Professor (retired), Department of Physics, ETH Zurich)
  • Formāts: Hardback, 302 pages, height x width x depth: 204x136x20 mm, weight: 716 g, 62 b/w illustrations
  • Izdošanas datums: 22-May-2014
  • Izdevniecība: Oxford University Press
  • ISBN-10: 0198705417
  • ISBN-13: 9780198705413
  • Hardback
  • Cena: 131,44 €
  • Grāmatu piegādes laiks ir 3-4 nedēļas, ja grāmata ir uz vietas izdevniecības noliktavā. Ja izdevējam nepieciešams publicēt jaunu tirāžu, grāmatas piegāde var aizkavēties.
  • Daudzums:
  • Ielikt grozā
  • Piegādes laiks - 4-6 nedēļas
  • Pievienot vēlmju sarakstam
  • Bibliotēkām
    • Oxford Scholarship Online e-books
  • Formāts: Hardback, 302 pages, height x width x depth: 204x136x20 mm, weight: 716 g, 62 b/w illustrations
  • Izdošanas datums: 22-May-2014
  • Izdevniecība: Oxford University Press
  • ISBN-10: 0198705417
  • ISBN-13: 9780198705413
In recent years, there have been important developments in the design and fabrication of new thermoelectrics. While a decade ago, progress was mainly empirical, recent advances in theoretical methods have led to a deeper understanding of the parameters that affect the performance of materials in thermoelectric devices. These have brought the goal of producing materials with the required characteristics for commercial application a significant step closer. A search for efficient materials requires a fully microscopic treatment of the charge and heat transport, and the aim of this book is to explain all thermoelectric phenomena from this modern quantum-mechanical perspective.

In the first part on phenomenology, conjugate current densities and forces are derived from the condition that the rate of change of the entropy density of the system in the steady state is given by the scalar product between them. The corresponding transport coefficients are explicitly shown to satisfy Onsager's reciprocal relations. The transport equations are solved for a number of cases, and the coefficient of performance, the efficiency, and the figure of merit are computed. State-of-the-art methods for the solution of the transport equations in inhomogeneous thermoelectrics are presented. A brief account on how to include magnetization transport in the formalism is also given.

In the second part, quantum mechanical expressions for the transport coefficients are derived, following the approach by Luttinger. These are shown to satisfy Onsager's relations by construction. Three lattice models, currently used to describe strongly correlated electron systems, are introduced: the Hubbard, the Falicov-Kimball, and the periodic Anderson model (PAM), and the relevant current density operators are derived for each of them. A proof of the Jonson-Mahan theorem, according to which all transport coefficients for these models can be obtained from the integral of a unique transport function multiplied by different powers of the frequency, is given.

The third part compares theory and experiment. First for the thermoelectric properties of dilute magnetic alloys, where the theoretical results are obtained from poor man's scaling solutions to single impurity models. Then it is shown that the experimental data on heavy fermions and valence fluctuators are well reproduced by the transport coefficients computed for the PAM at low and high temperature. Finally, results obtained from first principles calculations are shown, after a short introduction to density functional theory and beyond. A number of useful appendices complete the book.

Recenzijas

This book summarizes well the theoretical foundation of thermoelectricity, from classical thermodynamics to a modern quantum field treatment. The topics include detailed comparisons to experimental observation obtained from exquisite materials, such as Kondo materials and heavy fermion, together with first principle numerical approaches, providing a well-balanced monograph for modern theory of thermoelectricity. * Philip Kim, Columbia University *

1 Introduction
1(6)
PART I CLASSICAL THEORY
2 Phenomenological description of thermoelectric phenomena
7(6)
2.1 The entropy of a steady state
7(3)
2.2 Generalized currents and forces
10(1)
2.3 Transport equations and their symmetry
10(1)
2.4 A complete set of thermoelectric equations
11(2)
3 Phenomenological transport equations
13(4)
3.1 The charge current density--internal energy current density pair
13(1)
3.2 The charge current density--heat current density pair
14(2)
3.3 The charge current density--total energy current density pair
16(1)
4 Physical interpretation
17(5)
4.1 Thermoelectric heats
18(4)
5 Thermomagnetic and galvanomagnetic effects
22(9)
5.1 Transport equations in the presence of a uniform magnetic field
22(4)
5.2 Transport of magnetization
26(5)
6 Solutions of the transport equations for homogeneous thermoelectrics
31(9)
6.1 Homogeneous thermoelectrics with constant material parameters
31(3)
6.2 Figure of merit of the material
34(1)
6.3 Coefficient of performance
35(1)
6.4 Efficiency coefficient
36(1)
6.5 Homogeneous thermoelectrics with T-dependent material parameters
36(4)
7 Solutions of the transport equations for inhomogeneous thermoelectrics
40(12)
7.1 Segmented thermoelectrics
40(5)
7.2 Coefficient of performance, efficiency and figure of merit of a heterostructure with N segments
45(2)
7.3 Constrained-functional approach to device optimization
47(5)
8 Onsager's reciprocal relations in irreversible processes
52(13)
8.1 Thermodynamic description of fluctuations
52(6)
8.2 Statistical description of fluctuations
58(7)
PART II QUANTUM THEORY
9 Microscopic description of thermoelectric phenomena
65(7)
9.1 Slow and rapid perturbation
66(1)
9.2 Response to a diffusion force
66(3)
9.3 Response to a thermal force
69(3)
10 Calculation of the response to an applied field
72(10)
10.1 Linear response to an electrical force
72(4)
10.2 Linear response to a thermal force
76(2)
10.3 Equivalence to Kubo formula
78(4)
11 Current density operators
82(25)
11.1 Charge current density operators for continuous models
82(7)
11.2 Energy current density operators for continuous models
89(6)
11.3 Discrete models for the description of correlated systems
95(3)
11.4 Charge current density operators for discrete models
98(3)
11.5 Energy current density operators for discrete models
101(6)
12 Jonson-Mahan theorem
107(8)
PART III COMPARISON OF THEORY AND EXPERIMENT
13 Kondo effect in dilute alloys
115(27)
13.1 Introduction to the Kondo problem
115(2)
13.2 Experiments on dilute Kondo alloys
117(7)
13.3 Single-impurity models
124(5)
13.4 Solution of the Kondo problem by perturbative scaling
129(7)
13.5 Comparison of scaling results with experimental data
136(6)
14 Rare-earth intermetallics: heavy fermions and valence fluctuators
142(40)
14.1 High-temperature experiments
142(8)
14.2 Low-temperature experiments
150(3)
14.3 Theoretical description of heavy fermions and valence fluctuators at high temperature
153(12)
14.4 Theoretical description of heavy fermions and valence fluctuators at low temperature
165(3)
14.5 The Fermi liquid approach
168(8)
14.6 The Fermi liquid laws and the universal ratios
176(6)
15 First-principles approaches
182(33)
15.1 Bulk electron bands and phonon branches
182(7)
15.2 Bulk electronic transport coefficients
189(11)
15.3 Bulk lattice thermal conductivity
200(8)
15.4 Nanostructured materials
208(7)
APPENDICES
Appendix A Single-impurity models
215(12)
A.1 The orbitally degenerate Anderson model
215(2)
A.2 Crystal field effects
217(4)
A.3 From the Anderson to the s-d and Kondo Hamiltonians
221(4)
A.4 Orbital degeneracy, spin-orbit, and crystal field effects on the Kondo Hamiltonian
225(2)
Appendix B Green's functions
227(8)
B.1 Definitions
227(1)
B.2 Equations of motion and Fourier transforms
228(2)
B.3 Example 1: The single-impurity Anderson model (SIAM)
230(2)
B.4 Example 2: The periodic Anderson model (PAM)
232(3)
Appendix C Derivation of the spectral representation for the single-particle Green's function
235(3)
Appendix D Dynamical mean field theory of the PAM
238(3)
D.1 "Standard" mean field theory
238(1)
D.2 "Dynamical" mean field theory of the PAM
239(2)
Appendix E Scaling
241(9)
E.1 Elimination of high-energy conduction states
241(2)
E.2 Poor man's scaling for the Kondo model
243(3)
E.3 Analysis of the scaling equations
246(1)
E.4 Poor man's scaling for the Coqblin--Schrieffer model with crystal field splitting
247(3)
Appendix F Transport properties of dilute alloys
250(17)
F.1 Diagrammatic expansion
250(4)
F.2 Averaging over impurity configurations
254(3)
F.3 Lowest-order conductivity diagram
257(3)
F.4 Vertex corrections
260(1)
F.5 The &gammma;-vertex for Anderson impurities
261(3)
F.6 The partial wave analysis
264(3)
Appendix G Spectral function in the noncrossing approximation (NCA)
267(4)
Appendix H Correlation functions in the Fermi liquid regime: the DMFT solution
271(3)
Appendix I Sommerfeld expansion for heavy fermion systems in the DMFT approximation to the periodic Anderson model
274(5)
References 279(8)
Index 287
Born in 1945, Veljko Zlatic studied physics in Zagreb and obtained his first degree from Zagreb University in 1969. From 1970 to 1974 he studied theoretical physics at Imperial College and obtained his PhD. He taught many body physics at Zagreb University from 1974 to 1999. He was Humboldt Fellow at Frankfurt University in 1980/81 and Berlin University in 1989, Visiting Fellow at Oxford University in 1993/1994, and Visiting Professor at Georgetown University 1996/97 and 2006/07. He retired as a Senior Scientist from the Institute of Physics in 2010. His main research interest is the theoretical description of strongly correlated materials.

Born in 1946, René Monnier obtained his Diploma in Physics with honours from the University of Neuchātel in 1970. He was a Visiting Fellow at Cornell University from January 1971 to July 1972, after which he returned to Neuchātel, where he defended his thesis in April 1974. From October 1975 to July 1977 he was a postdoctoral fellow at Nordita, in Copenhagen. He joined ETH in October 1977 and was awarded the Professor title in 2000. His field of research is condensed matter theory, and his main interests lie in the study of the electronic structure and properties of random alloys and their surfaces, exotic compounds and strongly correlated systems. He has taught graduate courses on these subjects as well as introductory physics to students in engineering and in the life sciences.